<i>C</i> -axis textured M-type hexaferrite with tailored magnetic properties and narrow FMR linewidth for Ka-band self-biased circulator applications
Abstract
C-axis textured BaZn0.3Ti0.3Fe11.4O19 M-type hexaferrite was synthesized by solid-state reaction under magnetic field alignment, and its crystallographic site occupation, static and dynamic magnetic properties, and self-biased circulator performance were systematically investigated. At this intermediate substitution level, Rietveld refinement and Raman spectroscopy independently reveal that Zn2+–Ti4+ dopants are distributed across all five Fe3+ sublattices, with the 12k site accommodating the largest individual fraction—marking the onset of a multi-site substitution regime distinct from the selective 4f1/4f2 occupation dominant at lower doping levels. The saturation magnetization reaches 70.01 emu/g with a remanence ratio of 0.84, while the anisotropy field is reduced to 9871 Oe, reflecting a balance between the 4f1/4f2-driven anisotropy reduction and partial compensation by the 12k site. A narrow ferromagnetic resonance linewidth of 428 Oe is obtained at 58 GHz, and surface-integral analysis of the position-dependent demagnetizing factor demonstrates that finite-size-induced broadening contributes less than 9% to the measured linewidth. A slotted-structure self-biased circulator designed with the measured parameters exhibits a center frequency of 31.7 GHz and a 15-dB bandwidth of 2.3 GHz at the Ka-band. These results demonstrate that the intermediate-doping regime, wherein the 12k site becomes the primary dopant recipient, provides an effective route for simultaneously achieving a reduced anisotropy field and a narrow linewidth in substituted M-type hexaferrites for self-biased millimeter-wave circulator applications.
Article Details
Journal Info
Applied Physics Letters
American Institute of Physics
Authors (10)
Yongjie Liao
School of Mechanical and Electrical Engineering, Chengdu University of Technology 1 , Chengdu 610000,
Qian Liu
Ziyang Li
Key Laboratory of Micro and Nano Photonic Structures (MOE), School of Information Science and Technology
Xiao Tan
Yuxin Wu
Earth and Environmental Science Area, Lawrence Berkeley National Laboratory
Houjiao Chen
School of Mechanical and Electrical Engineering, Chengdu University of Technology 1 , Chengdu 610000,
Chang Li
Xin You
Center for Soft Condensed Matter Physics and Interdisciplinary Research & School of Physical Science and Technology
Chongsheng Wu
School of Mechanical and Electrical Engineering, Chengdu University of Technology 1 , Chengdu 610000,
Yuanming Lai
School of Mechanical and Electrical Engineering, Chengdu University of Technology 1 , Chengdu 610000,